TWI586986B - Magnetic sensor device - Google Patents
Magnetic sensor device Download PDFInfo
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- TWI586986B TWI586986B TW103103198A TW103103198A TWI586986B TW I586986 B TWI586986 B TW I586986B TW 103103198 A TW103103198 A TW 103103198A TW 103103198 A TW103103198 A TW 103103198A TW I586986 B TWI586986 B TW I586986B
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/12—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
- G01D5/14—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
- G01D5/142—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices
- G01D5/145—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices influenced by the relative movement between the Hall device and magnetic fields
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/0023—Electronic aspects, e.g. circuits for stimulation, evaluation, control; Treating the measured signals; calibration
- G01R33/0029—Treating the measured signals, e.g. removing offset or noise
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/02—Measuring direction or magnitude of magnetic fields or magnetic flux
- G01R33/06—Measuring direction or magnitude of magnetic fields or magnetic flux using galvano-magnetic devices
- G01R33/07—Hall effect devices
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03K—PULSE TECHNIQUE
- H03K17/00—Electronic switching or gating, i.e. not by contact-making and –breaking
- H03K17/94—Electronic switching or gating, i.e. not by contact-making and –breaking characterised by the way in which the control signals are generated
- H03K17/945—Proximity switches
- H03K17/95—Proximity switches using a magnetic detector
- H03K17/9517—Proximity switches using a magnetic detector using galvanomagnetic devices
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Description
本發明係關於將磁場強度轉換成電性訊號的磁性感測器裝置,例如關於利用於折疊式行動電話機或筆記型電腦等中之開關狀態檢測用感測器,或是馬達之旋轉位置檢測感測器等之磁性感測器裝置。 The present invention relates to a magnetic sensor device for converting a magnetic field strength into an electrical signal, for example, a sensor for detecting a switch state used in a foldable mobile phone or a notebook computer, or a sense of rotational position detection of a motor. A magnetic sensor device such as a detector.
就以摺疊式行動電話機或筆記型電腦等中之開關狀態檢測用感測器,或馬達之旋轉位置檢測感測器而言,使用有磁性感測器裝置。 A magnetic sensor device is used in the case of a switch state detecting sensor in a folding mobile phone or a notebook computer, or a rotational position detecting sensor of the motor.
磁性感測器裝置係藉由磁電轉換元件(例如霍耳元件)輸出與磁場強度或磁通密度呈比例之電壓,以放大器放大其輸出電壓,使用比較器而進行判定,以H訊號或L訊號之二值輸出。因磁電轉換元件之輸出電壓微小,故磁電轉換元件所持有之偏置電壓(元件偏置電壓),或放大器或比較器所持有之偏置電壓(輸入偏置電壓),再者磁性感測器裝置內之雜訊成為問題。元件偏置電壓主要係磁電轉換元件藉由封裝體所受到之應力等而產生。輸入偏置 電壓主要藉由構成放大器之輸入電路之元件的特性偏差等而產生。雜訊主要係藉由構成電路之單體電晶體所持有之閃爍雜音、單體電晶體或電阻元件所持有之熱雜音而產生。 The magnetic sensor device outputs a voltage proportional to the magnetic field strength or the magnetic flux density by a magnetoelectric conversion element (for example, a Hall element), amplifies the output voltage of the amplifier, and uses a comparator to determine the H signal or the L signal. The binary output. Since the output voltage of the magnetoelectric conversion element is small, the bias voltage (element bias voltage) held by the magnetoelectric conversion element, or the bias voltage (input bias voltage) held by the amplifier or the comparator, is magnetically sexy. The noise in the detector device becomes a problem. The component bias voltage is mainly generated by the magnetoelectric conversion element being subjected to stress or the like by the package. Input offset The voltage is mainly generated by a characteristic deviation or the like of an element constituting an input circuit of the amplifier. The noise is mainly generated by the scintillation noise, the single crystal or the thermal noise held by the resistive element held by the single crystal of the circuit.
提案有降低上述磁電轉換元件或放大器持有 之偏置電壓之影響的磁性感測器裝置(參照例如專利文獻1)。圖4所示之以往之磁性感測器裝置具備屬於磁電轉換元件之霍耳元件51、開關切換電路52、差動放大器53、比較器54、檢測電壓設定電路55、第一電容C51及第二電容C52、第一開關S51及第二開關S52。 Proposal to reduce the above magnetoelectric conversion element or amplifier holding A magnetic sensor device that affects the bias voltage (see, for example, Patent Document 1). The conventional magnetic sensor device shown in FIG. 4 includes a Hall element 51 belonging to a magnetoelectric conversion element, a switch switching circuit 52, a differential amplifier 53, a comparator 54, a detection voltage setting circuit 55, a first capacitor C51, and a second Capacitor C52, first switch S51 and second switch S52.
差動放大器53成為圖5所示之測量放大器構 成,具備差動放大器61、62和電阻R61、R62、R63。差動放大器61及62分別當作非反轉放大器而動作。差動放大器53之第一輸入端子被連接於差動放大器61之非反轉輸入端子E61,第二輸入端子被連接於差動放大器62之非反轉輸入端子E62,第一輸出端子被連接於差動放大器61之輸出端子E63,第二輸出端子被連接於差動放大器62之輸出端子E64。差動放大器53係藉由設成如此之測量放大器,而能夠抑制差動輸入中之同相雜訊的影響。在此,差動放大器61及62之放大率被設定成相等。 The differential amplifier 53 becomes the measuring amplifier structure shown in FIG. The differential amplifiers 61 and 62 and the resistors R61, R62, and R63 are provided. The differential amplifiers 61 and 62 operate as non-inverting amplifiers, respectively. The first input terminal of the differential amplifier 53 is connected to the non-inverting input terminal E61 of the differential amplifier 61, the second input terminal is connected to the non-inverting input terminal E62 of the differential amplifier 62, and the first output terminal is connected to The output terminal E63 of the differential amplifier 61 and the second output terminal are connected to the output terminal E64 of the differential amplifier 62. The differential amplifier 53 is capable of suppressing the influence of the in-phase noise in the differential input by providing such a measurement amplifier. Here, the amplification factors of the differential amplifiers 61 and 62 are set to be equal.
圖6表示以往之磁性感測器裝置之動作之時 序圖。檢測動作之一周期T係藉由上述開關切換電路52之動作,被區分成對霍耳元件51之第一端子對A-C輸入電源電壓,並從第二端子對B-D輸出檢測電壓之第一檢測 狀態T1,和對第二端子對B-D輸入電源電壓,並從第一端子對A-C輸出檢測電壓之第二檢測狀態T2。再者,藉由各開關之開關,區分成第1取樣相F1、第2取樣相F2、比較相F3。然後,在比較相F3中去除各偏置成分。 Figure 6 shows the operation of the conventional magnetic sensor device Sequence diagram. The one period T of the detecting operation is divided into the first terminal pair A-C input power supply voltage of the Hall element 51 and the first detection of the detection voltage from the second terminal pair B-D by the action of the above-described switch switching circuit 52. State T1, and a supply voltage to the second terminal pair B-D, and a second detection state T2 of the detection voltage is output from the first terminal pair A-C. Furthermore, the switches are divided into a first sampling phase F1, a second sampling phase F2, and a comparison phase F3. Then, each offset component is removed in the comparison phase F3.
[先行技術文獻] [Advanced technical literature]
[專利文獻] [Patent Literature]
[專利文獻1]日本特開2010-281801號公報 [Patent Document 1] Japanese Patent Laid-Open Publication No. 2010-281801
但是,在以往之磁性感測器裝置中,為了抵銷偏置成分,如取樣相(Sample Phase)和比較相般必須要有設置複數之訊號處理期間之時間分割動作,不適合高速訊號處理。再者,為了進行時間分割動作,必須要有開關電路或電容元件之連接,電路構成變得複雜。 However, in the conventional magnetic sensor device, in order to offset the offset component, such as the sample phase and the comparison phase, it is necessary to have a time division operation during which the signal processing period is set, which is not suitable for high-speed signal processing. Furthermore, in order to perform the time division operation, it is necessary to have a connection of a switching circuit or a capacitance element, and the circuit configuration becomes complicated.
本發明之目的在於提供藉由活用具有複數之霍耳元件和複數之差動輸入對的比較器,抵銷霍耳元件之偏置成分,實現高精度之磁場強度檢測,並且高速地進行訊號處理的磁性感測器裝置。 SUMMARY OF THE INVENTION It is an object of the present invention to provide a high precision magnetic field strength detection and high speed signal processing by utilizing a comparator having a plurality of Hall elements and a plurality of differential input pairs to offset the bias component of the Hall element. Magnetic sensor device.
為了解決以往般之問題點,本發明之磁性感 測器裝置構成下述般。 In order to solve the problem of the past, the magnetic sexy of the present invention The detector device is constructed as follows.
為一種磁性感測器裝置,具備:複數之霍耳元件、分別被連接於複數之霍耳元件的複數之可變電阻、分別連接複數之霍耳元件之複數的差動放大器、具有分別與複數之差動放大器連接的複數之差動輸入對的比較器。 A magnetic sensor device comprising: a plurality of Hall elements, a plurality of variable resistors respectively connected to a plurality of Hall elements, and a plurality of differential amplifiers respectively connected to the plurality of Hall elements, respectively having a complex number The comparator of the differential input pair of the differential amplifier is connected.
若藉由本發明之磁性感測器裝置時,因可以以小規模電路任意設定磁場強度之檢測電壓位準,故可取消霍耳元件偏置,並且可以高速地進行訊號處理。 According to the magnetic sensor device of the present invention, since the detection voltage level of the magnetic field strength can be arbitrarily set in a small-scale circuit, the Hall element offset can be canceled, and the signal processing can be performed at high speed.
1a、1b、51‧‧‧霍耳元件 1a, 1b, 51‧‧‧Horse components
2a、2b、53‧‧‧差動放大器 2a, 2b, 53‧‧‧Differential Amplifier
3、54‧‧‧比較器 3, 54‧‧‧ comparator
55‧‧‧檢測電壓設定電路 55‧‧‧Detection voltage setting circuit
52‧‧‧開關切換電路 52‧‧‧Switching circuit
Ra、Rb‧‧‧可變電阻 Ra, Rb‧‧‧Variable Resistors
圖1為表示本實施型態之磁性感測器裝置的電路圖。 Fig. 1 is a circuit diagram showing a magnetic sensor device of the present embodiment.
圖2為表示本實施型態之霍耳元件和可變電阻的電路圖。 Fig. 2 is a circuit diagram showing a Hall element and a variable resistor of the present embodiment.
圖3為本實施形態所使用之比較器之電路圖之一例。 Fig. 3 is an example of a circuit diagram of a comparator used in the embodiment.
圖4為以往之磁性感測器裝置之電路圖。 4 is a circuit diagram of a conventional magnetic sensor device.
圖5為以往之磁性感測器裝置之差動放大器之電路圖之一例。 Fig. 5 is a circuit diagram showing an example of a differential amplifier of a conventional magnetic sensor device.
圖6為以往之磁性感測器裝置之時序圖。 Fig. 6 is a timing chart of a conventional magnetic sensor device.
以下,針對本發明之實施形態一面參照圖面 一面予以詳細說明。本發明之磁性感測器裝置係作為折疊式行動電話機或筆記型電腦等中之開關狀態檢測感測器,或馬達之旋轉位置檢測感測器等,檢測磁場強度之狀態的感測器而被廣泛利用。在以下之實施型態中,雖然針對使用霍耳元件之磁性感測器裝置予以說明,但是本發明之磁性感測器裝置亦可以使用因應加速度或壓力等之各物理量而進行同樣的電壓輸出之轉換元件,來取代因應磁場強度而進行電壓輸出之霍耳元件。 Hereinafter, the embodiment of the present invention will be described with reference to the drawings. One side will explain in detail. The magnetic sensor device of the present invention is used as a sensor for detecting a state of a magnetic field strength as a switch state detecting sensor in a folding mobile phone or a notebook computer, or a rotational position detecting sensor of a motor or the like. Widely used. In the following embodiments, the magnetic sensor device using the Hall element is described. However, the magnetic sensor device of the present invention can perform the same voltage output in response to physical quantities such as acceleration or pressure. The conversion element replaces the Hall element that performs voltage output in response to the strength of the magnetic field.
圖1為表示與本發明有關之磁性感測器裝置 之實施形態的電路圖。本實施形態之磁性感測器裝置係由因應磁場強度而輸出訊號電壓之霍耳元件1a、1b、放大訊號電壓之差動放大器2a、2b、具有兩個差動輸入對之比較器3,和與霍耳元件連接之可變電阻Ra、Rb所構成。 1 is a view showing a magnetic sensor device related to the present invention A circuit diagram of an embodiment. The magnetic sensor device of the present embodiment is a Hall element 1a, 1b that outputs a signal voltage in response to a magnetic field strength, a differential amplifier 2a, 2b that amplifies a signal voltage, a comparator 3 having two differential input pairs, and The variable resistors Ra and Rb connected to the Hall element are formed.
霍耳元件1a、1b係在半導體基板上被配置分 別接近的位置上,連結霍耳元件1a之第一端子對A-C之直線,和連結霍耳元件1b之第一端子對E-G之直線被配置成互相平行之關係。其結果,連結霍耳元件1a之第二端子對B-D之直線,和連結霍耳元件1b之第二端子對F-H之直線也成為互相平行之關係。差動放大器2a、2b在以往例之說明中成為如圖5所示之測量放大器之構成。針對比較器3之詳細於後述,成為圖3所示之電路構成,輸出端子OUT之電壓VO以式(1)表示。 The Hall elements 1a and 1b are arranged on a semiconductor substrate. In a position that is not close, a straight line connecting the first terminal pair A-C of the Hall element 1a and a line connecting the first terminal pair E-G of the Hall element 1b are arranged in parallel relationship with each other. As a result, the straight line connecting the second terminal pair B-D of the Hall element 1a and the straight line connecting the second terminal pair F-H of the Hall element 1b are also in parallel relationship with each other. The differential amplifiers 2a and 2b have a configuration of a measuring amplifier as shown in FIG. 5 in the description of the conventional example. The details of the comparator 3 will be described later in the circuit configuration shown in FIG. 3, and the voltage VO of the output terminal OUT is expressed by the formula (1).
VO=A1(V6-V5)+A2(V8-V7)...(1) VO=A1(V6-V5)+A2(V8-V7). . . (1)
在此,A1、A2為構成比較器3之兩個差動放大器之各放大率。可變電阻Ra、Rb分別被連接於霍耳元件1a之差動放大器2a之一端子和接地間,霍耳元件1b之差動放大器2b之一端子和接地間。 Here, A1 and A2 are respective amplification factors of the two differential amplifiers constituting the comparator 3. The variable resistors Ra and Rb are respectively connected between one terminal of the differential amplifier 2a of the hall element 1a and the ground, and between one of the terminals of the differential amplifier 2b of the hall element 1b and the ground.
接著,針對本實施型態之磁性感測器裝置之動作予以說明。將霍耳元件1a、1b之輸出端子對中相對於磁場成分之差動輸出電壓設為Vh,將元件偏置電壓設為Voh,將同相電壓設為Vcm(≒VDD/2),將差動放大器2a、2b之各放大率設為G,將被輸出至以可變電阻Ra、Rb所決定之霍耳元件1a、1b之各輸出端子對的檢測電壓成分分別以Vrefa、Vrefb,針對訊號成分之傳達予以說明。因在霍耳元件1a和1b中,電流之流動方向旋轉90度,故霍耳元件1a之輸出端子對中之偏置成分和霍耳元件1b之輸出端子對中之偏置成分成為逆相。基於上述,當計算各連接點之訊號電壓時,則如同下述。 Next, the operation of the magnetic sensor device of the present embodiment will be described. The differential output voltage of the pair of output terminals of the Hall elements 1a and 1b with respect to the magnetic field component is Vh, the component bias voltage is Voh, and the in-phase voltage is Vcm (≒VDD/2), and the differential is The respective amplification factors of the amplifiers 2a and 2b are G, and the detection voltage components of the output terminal pairs of the Hall elements 1a and 1b determined by the variable resistors Ra and Rb are Vrefa and Vrefb, respectively, for the signal components. The communication is explained. Since the flow direction of the current is rotated by 90 degrees in the Hall elements 1a and 1b, the bias component of the pair of output terminals of the Hall element 1a and the bias component of the pair of output terminals of the Hall element 1b are reversed. Based on the above, when calculating the signal voltage of each connection point, it is as follows.
V1=Vcm-Vh/2+Voh/2...(2) V1=Vcm-Vh/2+Voh/2. . . (2)
V2=Vcm+Vh/2-Vrefa-Voh/2...(3) V2=Vcm+Vh/2-Vrefa-Voh/2. . . (3)
V3=Vcm-Vh/2-Voh/2...(4) V3=Vcm-Vh/2-Voh/2. . . (4)
V4=Vcm+Vh/2-Vrefb+Voh/2...(5) V4=Vcm+Vh/2-Vrefb+Voh/2. . . (5)
V5=Vcm-G(Vh/2-Voh/2)...(6) V5=Vcm-G(Vh/2-Voh/2). . . (6)
V6=Vcm+G(Vh/2-Vrefa-Voh/2)...(7) V6=Vcm+G(Vh/2-Vrefa-Voh/2). . . (7)
V7=Vcm-G(Vh/2+Voh/2)...(8) V7=Vcm-G(Vh/2+Voh/2). . . (8)
V8=Vcm+G(Vh/2-Vrefb+Voh/2)...(9) V8=Vcm+G(Vh/2-Vrefb+Voh/2). . . (9)
當將上述之V5~V8代入至式(1)時,電壓VO則以式(10)表示。在此,比較器3係各差動放大器持有同一性而 構成為一般,設為A1=A2=A。 When the above V5 to V8 are substituted into the equation (1), the voltage VO is expressed by the equation (10). Here, the comparator 3 is different in each differential amplifier. The configuration is generally set to A1=A2=A.
VO=AG(2Vh-Vrefa-Vrefb)...(10) VO=AG(2Vh-Vrefa-Vrefb). . . (10)
如此一來,可知霍耳元件1a、1b之偏置成分被抵銷,可以比較磁場強度之放大訊號成分和被任意設定之檢測電壓成分。在上述計算中,以分別在霍耳元件1a之端子B和接地間連接可變電阻Ra、在霍耳元件1b之端子G和接地間連接可變電阻Rb為前提,於可變電阻之一端之連接目的地從端子B切換至端子D,從端子G切換至端子E之時分別也取得相同之結果。此時,被檢測出之磁場強度之極性反轉。再者,在可變電阻之另一端之連接目的地從接地端子GND切換至電源電壓端子VDD之時,分別也取得相同之結果。 As a result, it can be seen that the offset components of the Hall elements 1a and 1b are offset, and the amplified signal component of the magnetic field strength and the arbitrarily set detection voltage component can be compared. In the above calculation, it is assumed that one of the variable resistors is connected to the variable resistor Ra between the terminal B of the hall element 1a and the ground, and the variable resistor Rb between the terminal G of the hall element 1b and the ground. The connection destination is switched from terminal B to terminal D, and the same result is obtained when switching from terminal G to terminal E. At this time, the polarity of the detected magnetic field intensity is reversed. Further, when the connection destination of the other end of the variable resistor is switched from the ground terminal GND to the power supply voltage terminal VDD, the same result is obtained.
在本實施形態中,電壓VO因係比較器(A之值非常大),故因應Vh之值,成為H訊號(VDD電位)或L訊號(GND電位)。再者,該些一連串之訊號處理無須如以往例般之時間分割訊號處理,可進行高速訊號處理。也不用於時間訊號處理之時所需要的開關電路或電容元件,可以縮小晶片尺寸,即是對於刪減成本也有貢獻。 In the present embodiment, since the voltage VO is a comparator (the value of A is very large), it is an H signal (VDD potential) or an L signal (GND potential) in response to the value of Vh. Moreover, the series of signal processing does not require time-division signal processing as in the prior art, and high-speed signal processing can be performed. It is also not used for the switching circuit or capacitor element required for time signal processing, which can reduce the size of the wafer, which is also contributing to the cost reduction.
在此,針對上述檢測電壓成分之Vrefa或Vrefb進行說明。如圖2所示般,霍耳元件1a、1b分別以由電阻R1~R4、R5~R8所構成之等效橋接電路所表示。可變電阻Ra係一端被連接於霍耳元件1a之端子B,另一端被連接於接地。同樣地,可變電阻Rb係一端被連接於 霍耳元件1b之端子G,另一端被連接於接地。接著,針對動作予以說明。在霍耳元件1a中端子B之電位和端子D之電位相等之時,即是,當考慮在後段之比較器中之第一差動輸入對之各電位相等之時,則成立式(11)之關係。 Here, Vrefa or Vrefb of the above-described detected voltage component will be described. As shown in Fig. 2, the Hall elements 1a and 1b are respectively represented by equivalent bridge circuits composed of resistors R1 to R4 and R5 to R8. One end of the variable resistor Ra is connected to the terminal B of the hall element 1a, and the other end is connected to the ground. Similarly, the variable resistor Rb is connected at one end to The terminal G of the Hall element 1b is connected to the ground at the other end. Next, the action will be described. When the potential of the terminal B and the potential of the terminal D are equal in the Hall element 1a, that is, when the potentials of the first differential input pair in the comparator of the subsequent stage are considered to be equal, the equation (11) is established. Relationship.
Ra=R1×R2×R3/(R2×R4-R1×R3).....(11) Ra = R1 × R2 × R3 / (R2 × R4 - R1 × R3). . . . . (11)
在此,在無磁場之狀態下,當被施加R1=R2=R3=R4=R,或某大小的磁場的狀態下之各電阻值之變動量設為△R時,在上述式(11)之狀態下,可以想成R1=R-△R、R2=R+△R、R3=R-△R、R4=R+△R。將該些代入式(11)時,則導出式(12)。 Here, in the state where no magnetic field is applied, when R1=R2=R3=R4=R, or a variation amount of each resistance value in a state of a magnetic field of a certain magnitude is ΔR, the above formula (11) In the state, it is conceivable that R1 = R - ΔR, R2 = R + ΔR, R3 = R - ΔR, and R4 = R + ΔR. When this is substituted into the formula (11), the formula (12) is derived.
Ra=R2(1-△R/R-(△R/R)2+(△R/R)3)/(4△R).....(12) Ra=R 2 (1-ΔR/R-(ΔR/R) 2 +(ΔR/R) 3 )/(4△R). . . . . (12)
因△R比R小很多,故當無視(△R/R)之二次、三次項時,則成立式(13)。 Since ΔR is much smaller than R, when the second or third term of (ΔR/R) is ignored, the equation (13) is established.
△R/R≒1/(1+4Ra/R).....(13) △R/R≒1/(1+4Ra/R). . . . . (13)
因此,在本實施形態中,不會依存電源電壓或製造偏差,可以僅以電阻比Ra/R決定檢測電壓。其結果,可以實現高精度之檢測電壓位準設定。同樣,即使在霍耳元件1b中,藉由可變電阻Rb同樣可以決定檢測電壓。藉由上述,檢測電壓成分Vrefa、Vrefb導出下述般。 Therefore, in the present embodiment, the detection voltage can be determined only by the resistance ratio Ra/R without depending on the power supply voltage or the manufacturing variation. As a result, a highly accurate detection voltage level setting can be achieved. Similarly, even in the Hall element 1b, the detection voltage can be determined by the variable resistor Rb. According to the above, the detected voltage components Vrefa and Vrefb are derived as follows.
Vrefa≒1/(1+4Ra/R)VDD.....(14) Vrefa≒1/(1+4Ra/R) VDD. . . . . (14)
Vrefb≒1/(1+4Rb/R)VDD.....(15) Vrefb≒1/(1+4Rb/R) VDD. . . . . (15)
再者,針對比較器3予以說明。比較器3成為圖3所示之電路構成,具有定電流電路I1、NMOS電晶體M43、M44A、M44B、M45A、M46A、M45B、M46B、PMOS電晶體M41、M42,被連接於下述般而構成。定電流電路I1之一方被連接於電源電壓端子VDD,另一方被連接於NMOS電晶體M43之汲極及閘極。將該連接點設為VBN。VBN被連接於NMOS電晶體M44A、M44B之各閘極。NMOS電晶體M43、M44A、M44B之源極被連接於接地端子VSS。NMOS電晶體M45A和M46A之源極被連接於M44A之汲極,NMOS電晶體M45B和M46B之源極被連接於M44B之汲極。NMOS電晶體M45A和M45B之汲極被連接於PMOS電晶體M41之汲極。將該連接點設為VA。NMOS電晶體M46A和M46B之汲極被連接於PMOS電晶體M42之汲極。該連接點被連接於比較器3之輸出端子OUT。PMOS電晶體M41和M42之閘極被連接於連接點VA,源極被連接於電源電壓端子VDD。NMOS電晶體M45A、M46A之閘極分別被連接於第一差動輸入對之第二輸入端子V6、第一輸入端子V5,NMOS電晶體M45B、M46B之閘極分別被連接於第二差動輸入對之第二輸入端子V8、第一輸入端子V7。 Furthermore, the comparator 3 will be described. The comparator 3 has a circuit configuration as shown in FIG. 3, and has a constant current circuit I1, NMOS transistors M43, M44A, M44B, M45A, M46A, M45B, M46B, and PMOS transistors M41 and M42, and is connected as follows. . One of the constant current circuits I1 is connected to the power supply voltage terminal VDD, and the other is connected to the drain and the gate of the NMOS transistor M43. Set this connection point to VBN. The VBN is connected to the gates of the NMOS transistors M44A, M44B. The sources of the NMOS transistors M43, M44A, and M44B are connected to the ground terminal VSS. The sources of the NMOS transistors M45A and M46A are connected to the drain of the M44A, and the sources of the NMOS transistors M45B and M46B are connected to the drain of the M44B. The drains of the NMOS transistors M45A and M45B are connected to the drain of the PMOS transistor M41. Set this connection point to VA. The drains of the NMOS transistors M46A and M46B are connected to the drain of the PMOS transistor M42. This connection point is connected to the output terminal OUT of the comparator 3. The gates of the PMOS transistors M41 and M42 are connected to the connection point VA, and the source is connected to the power supply voltage terminal VDD. The gates of the NMOS transistors M45A and M46A are respectively connected to the second input terminal V6 of the first differential input pair, the first input terminal V5, and the gates of the NMOS transistors M45B and M46B are respectively connected to the second differential input. The second input terminal V8 and the first input terminal V7.
接著,說明比較器3之動作。定電流電路I1係產生定電流,並供給至NMOS電晶體M43。NMOS電晶 體M43、M44A、M44B構成電流鏡電路,在NMOS電晶體M44A、M44B之汲極-源極間流通根據在M43之汲極-源極間流動之電流的電流。由NMOS電晶體M44A、M45A、M46A、PMOS電晶體M41、M42所構成之5個電晶體構成差動放大器,放大NMOS電晶體M45A、M46A之閘極電壓之差,即是第一差動輸入對之第二輸入端子V6和第一輸入端子V5之電壓差,而動作成輸出至輸出端子OUT。將該放大率設為A1。在此,針對電流鏡電路構成及差動放大器構成之動作,在CMOS類比電路之文獻等中有詳細記載,在此省略詳細之說明。再者,由NMOS電晶體M44B、M45B、M46B、PMOS電晶體M41、M42所構成之5個電晶體構成差動放大器,放大NMOS電晶體M45B、M46B之閘極電壓之差,即是第二差動輸入對之第二輸入端子V8和第一輸入端子V7之電壓差,而動作成輸出至輸出端子OUT。將該放大率設為A2。再者,NMOS電晶體M45A、M45B之各汲極在連接點VA被連接於PMOS電晶體M41之汲極,NMOS電晶體M46A、M46B之各汲極在輸出端子OUT被連接於PMOS電晶體M42之汲極,依此在該連接點VA及輸出端子VO,動作成被加算被輸入至各差動放大器且被放大的訊號電壓。將該些動作以式表示,則如同上述式(1)般。 Next, the operation of the comparator 3 will be described. The constant current circuit I1 generates a constant current and supplies it to the NMOS transistor M43. NMOS transistor The bodies M43, M44A, and M44B constitute a current mirror circuit, and a current flowing according to a current flowing between the drain and the source of M43 flows between the drain and the source of the NMOS transistors M44A and M44B. The five transistors formed by the NMOS transistors M44A, M45A, M46A, and the PMOS transistors M41 and M42 constitute a differential amplifier, and the difference between the gate voltages of the NMOS transistors M45A and M46A is amplified, that is, the first differential input pair. The voltage difference between the second input terminal V6 and the first input terminal V5 acts to output to the output terminal OUT. This magnification is set to A1. Here, the operation of the configuration of the current mirror circuit and the configuration of the differential amplifier is described in detail in the literature of the CMOS analog circuit, and the detailed description thereof is omitted here. Furthermore, the five transistors composed of the NMOS transistors M44B, M45B, M46B, and the PMOS transistors M41 and M42 constitute a differential amplifier, and the difference between the gate voltages of the NMOS transistors M45B and M46B is a second difference. The voltage input difference between the second input terminal V8 and the first input terminal V7 is input to the output terminal OUT. This magnification is set to A2. Furthermore, the drains of the NMOS transistors M45A and M45B are connected to the drain of the PMOS transistor M41 at the connection point VA, and the drains of the NMOS transistors M46A and M46B are connected to the PMOS transistor M42 at the output terminal OUT. In this case, the connection point VA and the output terminal VO operate as a signal voltage that is input to each differential amplifier and amplified. These actions are expressed by the equation, as in the above formula (1).
並且,關於本實施形態,將霍耳元件及可變電阻分別增加例如各四個,而配合此將比較器之差動輸入對增加至四個(8個輸入端子),依此可以更抑制霍耳元件 偏置偏差之影響,亦可更提高磁場強度之檢測精度。如此一來,本發眀可以對應於活用具有複數霍耳元件和複數之差動輸入對之比較器的構成。 Further, in the present embodiment, the Hall element and the variable resistor are respectively increased by, for example, four, and the differential input pair of the comparator is increased to four (8 input terminals), thereby suppressing the Huo Ear element The influence of the offset deviation can also improve the detection accuracy of the magnetic field strength. As such, the present invention can correspond to the construction of a comparator having a plurality of Hall elements and a plurality of differential input pairs.
再者,在本發眀之實施形態中所示之磁性感測器裝置藉由將比較器變更成差動放大器,亦可以成為輸出類比訊號之構成。 Furthermore, the magnetic sensor device shown in the embodiment of the present invention can also be configured as an output analog signal by changing the comparator to a differential amplifier.
1a、1b‧‧‧霍耳元件 1a, 1b‧‧‧Horse components
2a、2b‧‧‧差動放大器 2a, 2b‧‧‧Differential Amplifier
3‧‧‧比較器 3‧‧‧ comparator
Ra、Rb‧‧‧可變電阻 Ra, Rb‧‧‧Variable Resistors
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